Avago Technologies ACPL-C870-000E User Manual

EVBD-ACPL-C87B/C87A/C870
Isolated Voltage Sensor Evaluation Board
User Guide
Board Description
The ACPL-C87x evaluation board (see Figure 1 and Fig­ure 2) is designed to support the evaluation of the AC­PL-C87x precision optically isolated voltage sensors. The ACPL-C87x series is available in three choices: ACPL-C87B (±0.5% gain tolerance), ACPL-C79A (±1% gain tolerance) and ACPL-C790 (±3% gain tolerance). Featuring 2 V put range and 1 G high input impedance, these isolation ampliers are specically designed for voltage sensing in electronic power converters applications, including motor drives and renewable energy systems. The ACPL-C87x is identied as U1 on the evaluation board.
On the input side of the evaluation board, power terminals P1 and P2 are provided for incoming voltage connection. This voltage is required to scale down to suit the input range of the voltage senor. This can be achieved by choos­ing appropriate resistors and mount on the footprints pro­vided for R1 through R3. On the output side of the evalu­ation board, header connector P7 provides a connection port for power supply to the board and signal interface with next stage such as an analog to digital converter or a signal processing and control device.
Note:
1. The ACPL-C87x data sheet species 2 V as the nominal input range. Full scale input range (FSR) is 2.46 V.
[1]
in-
Features
User-congurable voltage sensing range up to 1230 V
Single 5 V supply or dual supply up to ±15 V
Onboard oset calibration
Onboard isolated 5 V power supply for high voltage
User-controllable shutdown
Voltage Sensor Applications
Isolated voltage sensing in AC and servo motor drives
Isolated DC-bus voltage sensing in solar inverters, wind
turbine inverters
Isolated sensor interfaces
Signal Isolation in data acquisition systems
General purpose voltage isolation
Figure 1. The ACPL-C87x evaluation board (top view)
Figure 2. The ACPL-C87x evaluation board (bottom view)
Schematic
Figure 3 shows the evaluation board schematic. In a typical voltage sensing implementation, a resistive voltage divider is used to scale the DC-link voltage to suit the input range of the voltage sensor. Power terminals P1 and P2 are used to connect to the DC-link voltage across nodes L1 and L2 to be monitored. This voltage, denoted as VL1 as L2 is connected to the reference point GND1, is scaled down through a resistive divider consists of resistors R1 through R4 in series. On this board, R4 has a xed value of 10 k, although it can be replaced by another value, if desired.
VDD2
GND1
C1
22 nF
GND1
C2 100 nF
TP5
C3
0.47 µF
VDD1
GND1
GND1
0.47
µF
C4
GND2
1
C5
100 nF
TP7
TP6
R6
700
U6
OUT
GND
7
6
LM78L05ACM
10K, 1%
R7 R8
10K, 1%
C6
1 nF
GND2
3
SHDN
2
C7
1 nF
VDD2
GND2
V+
8
IN
C10 100 nF
GND2
1 nFC8
1 nFC9
R10
10K, 1%
R9
10K, 1%
V
ref
REF-SEL
GND2
P3
1 2 3
Jumper default position: Pin 1-2
0.1 µFC11
2
7
6
3
4
VS-_SEL
C12
P4
1
GND2
2 3
Jumper default position: Pin 1-2
GND2
VS+_SEL
V+
U4 OPA237UA
V-
U3
5
+V
out
7
-V
out
NKE0505DC
U1
1
V
DD1
2
V
IN
3
SHDN
4
GND1
ACPL-C87X
U2
4
GND
5
V
O
6
V
CC
ACPL-W50L
+V
in
-V
in
V
DD2
V
OUT+
V
OUT-
GND2
CATHODE
ANODE
4
1
GND2
VDD2
8
7
6
5
GND2
3
2
NC
1
P1
2 1
Power Terminal
P2
2 1
Power Terminal
Put an area of through-holes for prototyping
TP1
TP2
L1
R1 Leave blank
R2 Leave blank
R3
TP3
Leave blank
R4
TP4
10k, 1%
L2
R5
10k
VDD1
Figure 3. The ACPL-C87x evaluation board schematic
Given that the voltage sensor ACPL-C87x’s nominal input voltage for VIN is 2 V, a user needs to choose resistors R1, R2 and R3 according to Equation 1.
R11 1K
GND2
C13
1 µF
VDD2
GND2
V
= 0.4V*(1+(R12+R
ref
U5
IN4OUT
3
DNC
2
P5
1 2 3
Jumper default position: Pin 1-2
P6
1 2 3
Jumper default position: Pin 1-2
GND
LT6650CS5(IS5)
TP8
V
out
FB
)/R14) = 0.48 to 0.52 V
Pot
5
C14
1 nF
1
V
GND2
GND2
SHDN
GND2
V
ref
3
GND2
DD2
V+
V-
V V
C15
R12
1 µF
20K
GND2
1
R13 R
10k
Pot
2
R14 100K
P7
1 2 3 4 5 6
out
7
ref
8 9 10
Header
- Equation 1
For example, if VL1 = 600 V, then the combined value of R1, R2 and R3 = 2990 k.
Choosing resistors is exible. One method is to combine several resistors to match the target value; e.g., 2 M, 430 k and 560 k resistors make up 2990 k exactly. In this way, VIN of 2 V corresponds to VL1 of 600 V. However, in the cases that VL1 has a dierent value from 600 V, specic resistance values might be dicult to nd. Another method is to round up the target value to a convenient value 3 M to make choosing resistors easier; e.g., 1 M is a common value and 3 pieces of it make 3 M. In this way, the scaling relationship needs some ne tune. In the same example with VL1 = 600 V, R1+R2+R3 = 3 M, and R4 = 10 k, VIN is solved to be 1.993 V.
After deciding resistance for R1 through R3, surface mount type devices can be mounted on the footprints provided. In case only through-hole type resistors are available, the prototyping area can be used instead.
The down-scaled input voltage is ltered by the anti-aliasing lter formed by R4 and C1 with corner frequency of 723 Hz
[1]
and then sensed by the ACPL-C87x. A dierential output voltage that is proportional to the input voltage is created
on the other side of the optical isolation barrier.
Note: 1. The total value of R1 through R3 in series is usually much larger than R4, therefore neglected in calculation.
Following the isolation amplier, an OPA237 congured as a dierence amplier converts the dierential signal to a single-ended output. This stage can be congured to further amplify the signal, if required, and form a low-pass lter to limit the bandwidth. In this circuit, the dierence amplier is designed for a gain of 1 with a low-pass lter corner fre­quency of 8 kHz. Resistors R9 and R10 can be selected for a dierent gain. The bandwidth can be reduced by increasing capacitance for C6 and C8.
2
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